Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens can have negative refractive force. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imaging quality for use in compact cameras.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and more particularly to a compact optical image capturing system for an electronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of the ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of the pixel size of the image sensing device, the development of the optical image capturing system towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The conventional optical system of the portable electronic device usually has five or six lenses. However, the optical system is asked to take pictures in a dark environment, in other words, the optical system is asked to have a large aperture. The conventional optical system could not provide a high optical performance as required.

It is an important issue to increase the amount of light entering the lens. In addition, the modern lens is also asked to have several characters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of seven-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the amount of incoming light of the optical image capturing system, and to improve imaging quality for image formation, so as to be applied to minimized electronic products.

In addition, when it comes to certain application of optical imaging, there will be a need to capture image via light sources with wavelengths in both visible and infrared ranges, an example of this kind of application is IP video surveillance camera, which is equipped with the Day & Night function. The visible spectrum for human vision has wavelengths ranging from 400 to 700 nm, but the image formed on the camera sensor includes infrared light, which is invisible to human eyes. Therefore, under certain circumstances, an IR cut filter removable (ICR) is placed before the sensor of the IP video surveillance camera, in order to ensure that only the light that is visible to human eyes is picked up by the sensor eventually, so as to enhance the “fidelity” of the image. The ICR of the IP video surveillance camera can completely filter out the infrared light under daytime mode to avoid color cast; whereas under night mode, it allows infrared light to pass through the lens to enhance the image brightness. Nevertheless, the elements of the ICR occupy a significant amount of space and are expensive, which impede to the design and manufacture of miniaturized surveillance cameras in the future.

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which utilize the combination of refractive powers, convex surfaces and concave surfaces of four lenses, as well as the selection of materials thereof, to reduce the difference between the imaging focal length of visible light and imaging focal length of infrared light, in order to achieve the near “confocal” effect without the use of ICR elements.

The term and its definition to the lens parameter in the embodiment of the present are shown as below for further reference.

The lens parameters related to the magnification of the optical image capturing system

The optical image capturing system can be designed and applied to biometrics, for example, facial recognition. When the embodiment of the present disclosure is configured to capture image for facial recognition, the infrared light can be adopted as the operation wavelength. For a face of about 15 centimeters (cm) wide at a distance of 25-30 cm, at least 30 horizontal pixels can be formed in the horizontal direction of an image sensor (pixel size of 1.4 micrometers (μm)). The linear magnification of the infrared light on the image plane is LM, and it meets the following conditions: LM≤0.0003, where LM=(30 horizontal pixels)*(1.4 μm pixel size)/(15 cm, width of the photographed object). Alternatively, the visible light can also be adopted as the operation wavelength for image recognition. When the visible light is adopted, for a face of about 15 cm wide at a distance of 25-30 cm, at least 50 horizontal pixels can be formed in the horizontal direction of an image sensor (pixel size of 1.4 micrometers (μm)).

The lens parameter related to a length or a height in the lens:

For visible spectrum, the present invention may adopt the wavelength of 555 nm as the primary reference wavelength and the basis for the measurement of focus shift; for infrared spectrum (700-1000 nm), the present invention may adopt the wavelength of 850 nm as the primary reference wavelength and the basis for the measurement of focus shift.

The optical image capturing system includes a first image plane and a second image plane. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value in the central of field of view of the second image plane. The optical image capturing system also includes a first average image plane and a second average image plane. The first average image plane is an image plane specifically for the visible light, and the first average image plane is perpendicular to the optical axis. The first average image plane is installed at the average position of the defocusing positions, where the values of MTF of the visible light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The second average image plane is an image plane specifically for the infrared light, and the second average image plane is perpendicular to the optical axis. The second average image plane is installed at the average position of the defocusing positions, where the values of MTF of the infrared light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency.

The aforementioned first spatial frequency is set to be half of the spatial frequency (half frequency) of the image sensor (sensor) used in the present invention. For example, for an image sensor having the pixel size of 1.12 μm or less, one-eighth of the spatial frequency, the quarter spatial frequency, half spatial frequency (half frequency) and full spatial frequency (full frequency) in the characteristic diagram of modulation transfer function are at least 55 cycles/mm, 110 cycles/mm, 220 cycles/mm and 440 cycles/mm, respectively. Lights of any field of view can be further divided into sagittal ray and tangential ray.

The focus shifts where the through-focus MTF values of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VSFS0, VSFS3, and VSFS7 (unit of measurement: mm), respectively. The maximum values of the through-focus MTF of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7, respectively. The focus shifts where the through-focus MTF values of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VTFS0, VTFS3, and VTFS7 (unit of measurement: mm), respectively. The maximum values of the through-focus MTF of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively. The average focus shift (position) of both the aforementioned focus shifts of the visible sagittal ray at three fields of view and focus shifts of the visible tangential ray at three fields of view is denoted by AVFS (unit of measurement: mm), which equals to the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|.

The focus shifts where the through-focus MTF values of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit of measurement: mm), respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared sagittal ray at three fields of view is denoted by AISFS (unit of measurement: mm). The maximum values of the through-focus MTF of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The focus shifts where the through-focus MTF values of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm), respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared tangential ray at three fields of view is denoted by AITFS (unit of measurement: mm). The maximum values of the through-focus MTF of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, and ITMTF7, respectively. The average focus shift (position) of both of the aforementioned focus shifts of the infrared sagittal ray at the three fields of view and focus shifts of the infrared tangential ray at the three fields of view is denoted by AIFS (unit of measurement: mm), which equals to the absolute value of |(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6.

The focus shift (difference) between the focal points of the visible light and the infrared light at their central fields of view (RGB/IR) of the entire optical image capturing system (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm) is denoted by FS, which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|. The difference (focus shift) between the average focus shift of the visible light in the three fields of view and the average focus shift of the infrared light in the three fields of view (RGB/IR) of the entire optical image capturing system is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm), which equals to the absolute value of |AIFS−AVFS|.

A maximum height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens to the image-side surface of the seventh lens is denoted by InTL. A distance from the first lens to the second lens is denoted by IN12 (instance). A central thickness of the first lens of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens is denoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system is denoted by HEP. For any surface of any lens, a maximum effective half diameter (EHD) is a perpendicular distance between an optical axis and a crossing point on the surface where the incident light with a maximum viewing angle of the system passing the very edge of the entrance pupil. For example, the maximum effective half diameter of the object-side surface of the first lens is denoted by EHD11, the maximum effective half diameter of the image-side surface of the first lens is denoted by EHD12, the maximum effective half diameter of the object-side surface of the second lens is denoted by EHD21, the maximum effective half diameter of the image-side surface of the second lens is denoted by EHD22, and so on.

The lens parameter related to an arc length of the shape of a surface and a surface profile:

For any surface of any lens, a profile curve length of the maximum effective half diameter is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to an end point of the maximum effective half diameter thereof. In other words, the curve length between the aforementioned start and end points is the profile curve length of the maximum effective half diameter, which is denoted by ARS. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, the profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of the entrance pupil diameter (HEP) is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis. In other words, the curve length between the aforementioned stat point and the coordinate point is the profile curve length of a half of the entrance pupil diameter (HEP), and is denoted by ARE. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A displacement from a point on the object-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the object-side surface of the seventh lens ends, is denoted by InRS71 (the depth of the maximum effective semi diameter). A displacement from a point on the image-side surface of the seventh lens, which is passed through by the optical axis, to a point on the optical axis, where a projection of the maximum effective semi diameter of the image-side surface of the seventh lens ends, is denoted by InRS72 (the depth of the maximum effective semi diameter). The depth of the maximum effective semi diameter (sinkage) on the object-side surface or the image-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. By the definition, a distance perpendicular to the optical axis between a critical point C51 on the object-side surface of the fifth lens and the optical axis is HVT51 (instance), and a distance perpendicular to the optical axis between a critical point C52 on the image-side surface of the fifth lens and the optical axis is HVT52 (instance). A distance perpendicular to the optical axis between a critical point C61 on the object-side surface of the sixth lens and the optical axis is HVT61 (instance), and a distance perpendicular to the optical axis between a critical point C62 on the image-side surface of the sixth lens and the optical axis is HVT62 (instance). A distance perpendicular to the optical axis between a critical point on the object-side or image-side surface of other lenses, e.g., the seventh lens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection point IF711 which is nearest to the optical axis, and the sinkage value of the inflection point IF711 is denoted by SGI711 (instance). A distance perpendicular to the optical axis between the inflection point IF711 and the optical axis is HIF711 (instance). The image-side surface of the seventh lens has one inflection point IF721 which is nearest to the optical axis, and the sinkage value of the inflection point IF721 is denoted by SGI721 (instance). A distance perpendicular to the optical axis between the inflection point IF721 and the optical axis is HIF721 (instance).

The object-side surface of the seventh lens has one inflection point IF712 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF712 is denoted by SGI712 (instance). A distance perpendicular to the optical axis between the inflection point IF712 and the optical axis is HIF712 (instance). The image-side surface of the seventh lens has one inflection point IF722 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF722 is denoted by SGI722 (instance). A distance perpendicular to the optical axis between the inflection point IF722 and the optical axis is HIF722 (instance).

The object-side surface of the seventh lens has one inflection point IF713 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF713 is denoted by SGI713 (instance). A distance perpendicular to the optical axis between the inflection point IF713 and the optical axis is HIF713 (instance). The image-side surface of the seventh lens has one inflection point IF723 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF723 is denoted by SGI723 (instance). A distance perpendicular to the optical axis between the inflection point IF723 and the optical axis is HIF723 (instance).

The object-side surface of the seventh lens has one inflection point IF714 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF714 is denoted by SGI714 (instance). A distance perpendicular to the optical axis between the inflection point IF714 and the optical axis is HIF714 (instance). The image-side surface of the seventh lens has one inflection point IF724 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF724 is denoted by SGI724 (instance). A distance perpendicular to the optical axis between the inflection point IF724 and the optical axis is HIF724 (instance).

An inflection point, a distance perpendicular to the optical axis between the inflection point and the optical axis, and a sinkage value thereof on the object-side surface or image-side surface of other lenses is denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100% field. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, which stands for STOP transverse aberration, and is used to evaluate the performance of one specific optical image capturing system. The transverse aberration of light in any field of view can be calculated with a tangential fan or a sagittal fan. More specifically, the transverse aberration caused when the longest operation wavelength (e.g., 650 nm) and the shortest operation wavelength (e.g., 470 nm) pass through the edge of the aperture can be used as the reference for evaluating performance. The coordinate directions of the aforementioned tangential fan can be further divided into a positive direction (upper light) and a negative direction (lower light). The longest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the reference wavelength of the mail light (e.g., 555 nm) has another imaging position on the image plane in the same field of view. The transverse aberration caused when the longest operation wavelength passes through the edge of the aperture is defined as a distance between these two imaging positions. Similarly, the shortest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the transverse aberration caused when the shortest operation wavelength passes through the edge of the aperture is defined as a distance between the imaging position of the shortest operation wavelength and the imaging position of the reference wavelength. The performance of the optical image capturing system can be considered excellent if the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view (i.e., 0.7 times the height for image formation HOI) are both less than 100 μm. Furthermore, for a stricter evaluation, the performance cannot be considered excellent unless the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on the image plane vertical to the optical axis. A transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by PLTA; a transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by PSTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by NLTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by NSTA; a transverse aberration at 0.7 HOI of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by SLTA; a transverse aberration at 0.7 HOI of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system capable of focusing visible and infrared light (i.e., dual-mode) at the same time and achieving certain performance, in which the seventh lens is provided with an inflection point at the object-side surface or at the image-side surface to adjust the incident angle of each view field and modify the ODT and the TDT. In addition, the surfaces of the seventh lens are capable of modifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, as sixth lens, a seventh lens, a first image plane, and a second image plane. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central of field of view of the second image plane. All lenses among the first lens to the seventh lens have refractive power. The optical image capturing system satisfies:

1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; |FS|≤60 μm; and 1≤HOS/HOI≤15;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first, the second, the third, the fourth, the fifth, the sixth, the seventh lenses, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance between the object-side surface of the first lens and the first image plane on the optical axis; HAF is a half of a maximum view angle of the optical image capturing system; HOI is the maximum image height on the first image plane perpendicular to the optical axis of the optical image capturing system; FS is the distance on the optical axis between the first image plane and the second image plane.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, a first image plane, and a second image plane. The first image plane is an image plane specifically for the visible light, and the first image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central field of view of the first image plane; the second image plane is an image plane specifically for the infrared light, and second image plane is perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency has a maximum value at the central of field of view of the second image plane. The first lens has refractive power, and the object-side surface thereof can be convex near the optical axis. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power. HO is a maximum height for image formation perpendicular to the optical axis on the image plane. At least one lens among the first lens to the seventh lens has positive refractive power. The optical image capturing system satisfies:

1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; |FS|≤30 μm; 1≤(ARE/HEP)≤2.0; and 1≤HOS/HOI≤15;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first, the second, the third, the fourth, the fifth, the sixth, the seventh lenses, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance between the object-side surface of the first lens and the first image plane on the optical axis; HAF is a half of a maximum view angle of the optical image capturing system; HOI is the maximum image height on the first image plane perpendicular to the optical axis of the optical image capturing system; FS is the distance on the optical axis between the first image plane and the second image plane; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis. At least one lens among the first lens to the seventh lens is made of glass.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, a first average image plane, and a second average image plane. The first average image plane is an image plane specifically for the visible light, and the first average image plane is perpendicular to the optical axis. The first average image plane is installed at the average position of the defocusing positions, where the values of MTF of the visible light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The second average image plane is an image plane specifically for the infrared light, and the second average image plane is perpendicular to the optical axis. The second average image plane is installed at the average position of the defocusing positions, where the values of MTF of the infrared light at the central field of view, 0.3 field of view, and the 0.7 field of view are at their respective maximum at the first spatial frequency. The number of the lenses having refractive power in the optical image capturing system is seven. HOI is a maximum height for image formation perpendicular to the optical axis on the image plane. At least one lens among the first lens to the seventh lens is made of glass. The first lens has refractive power. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power. At least one lens among the first lens to the seventh lens has positive refractive power. The optical image capturing system satisfies:

1≤f/HEP≤10; 0 deg<HAF≤150 deg; |AFS|≤30 μm; 1≤2(ARE/HEP)≤2.0; and 1≤HOS/HOI≤10;

where f1, f2, f3, f4, f5, f6, and f7 are the focal lengths of the first, the second, the third, the fourth, the fifth, the sixth, the seventh lenses, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance between the object-side surface of the first lens and the first average image plane on the optical axis; HAF is a half of a maximum view angle of the optical image capturing system; HOI is the maximum image height on the first average image plane perpendicular to the optical axis of the optical image capturing system; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; AFS is the distance between the first average image plane and the second average image plane.

For any surface of any lens, the profile curve length within the effective half diameter affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within the effective half diameter of any surface of any lens has to be controlled. The ratio between the profile curve length (ARS) within the effective half diameter of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARS/TP) has to be particularly controlled. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARS11/TP1; the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, and the ratio between ARS12 and TP1 is ARS12/TP1. The profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARS21/TP2; the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of the maximum effective half diameter thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

For any surface of any lens, the profile curve length within a half of the entrance pupil diameter (HEP) affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within a half of the entrance pupil diameter (HEP) of any surface of any lens has to be controlled. The ratio between the profile curve length (ARE) within a half of the entrance pupil diameter (HEP) of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARE/TP) has to be particularly controlled. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARE11/TP1; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, and the ratio between ARE12 and TP1 is ARE12/TP1. The profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARE21/TP2; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of a half of the entrance pupil diameter (HEP) thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS) can be reduced while |f1|>f7.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of the lenses satisfy the aforementioned conditions, at least one lens among the second to the sixth lenses could have weak positive refractive power or weak negative refractive power. Herein the weak refractive power means the absolute value of the focal length of one specific lens is greater than 10. When at least one lens among the second to the sixth lenses has weak positive refractive power, it may share the positive refractive power of the first lens, and on the contrary, when at least one lens among the second to the sixth lenses has weak negative refractive power, it may fine turn and correct the aberration of the system.

In an embodiment, the seventh lens could have negative refractive power, and an image-side surface thereof is concave, it may reduce back focal length and size. Besides, the seventh lens can have at least an inflection point on at least a surface thereof, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to the following detailed description of some illustrative embodiments in conjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the present invention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the first embodiment of the present application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 1D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present invention;

FIG. 1E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present disclosure;

FIG. 2A is a schematic diagram of a second embodiment of the present invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the second embodiment of the present application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical image capturing system of the second embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 2D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present invention;

FIG. 2E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present disclosure;

FIG. 3A is a schematic diagram of a third embodiment of the present invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the third embodiment of the present application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical image capturing system of the third embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 3D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present invention;

FIG. 3E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present disclosure;

FIG. 4A is a schematic diagram of a fourth embodiment of the present invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fourth embodiment of the present application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical image capturing system of the fourth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 4D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present invention;

FIG. 4E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present disclosure;

FIG. 5A is a schematic diagram of a fifth embodiment of the present invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fifth embodiment of the present application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical image capturing system of the fifth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 5D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present invention;

FIG. 5E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present disclosure;

FIG. 6A is a schematic diagram of a sixth embodiment of the present invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the sixth embodiment of the present application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical image capturing system of the sixth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 6D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present invention; and

FIG. 6E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present disclosure.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane from an object side to an image side. The optical image capturing system further is provided with an image sensor at an image plane. The height for image formation in each of the following embodiments is about 3.91 mm.

The optical image capturing system can work in three wavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters. The optical image capturing system can also work in five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650 nm wherein 555 nm is the main reference wavelength, and is the reference wavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies 0.5≤ΣPPR/|ΣNPR|≤15, and a preferable range is 1≤ΣPPR/|ΣNPR|≤3.0, where PPR is a ratio of the focal length fp of the optical image capturing system to a focal length fp of each of lenses with positive refractive power; NPR is a ratio of the focal length fn of the optical image capturing system to a focal length fn of each of lenses with negative refractive power; ΣPPR is a sum of the PPRs of each positive lens; and ΣNPR is a sum of the NPRs of each negative lens. It is helpful for control of an entire refractive power and an entire length of the optical image capturing system.

The image sensor is provided on the image plane. The optical image capturing system of the present invention satisfies HOS/HOI≤10 and 0.5≤HOS/f≤10, and a preferable range is 1≤HOS/HOI≤5 and 1≤HOS/f≤7, where HOI is a half of a diagonal of an effective sensing area of the image sensor, i.e., the maximum image height, and HOS is a height of the optical image capturing system, i.e. a distance on the optical axis between the object-side surface of the first lens and the image plane. It is helpful for reduction of the size of the system for used in compact cameras.

The optical image capturing system of the present invention further is provided with an aperture to increase image quality.

In the optical image capturing system of the present invention, the aperture could be a front aperture or a middle aperture, wherein the front aperture is provided between the object and the first lens, and the middle is provided between the first lens and the image plane. The front aperture provides a long distance between an exit pupil of the system and the image plane, which allows more elements to be installed. The middle could enlarge a view angle of view of the system and increase the efficiency of the image sensor. The optical image capturing system satisfies 0.2≤InS/HOS≤1.1, where InS is a distance between the aperture and the image-side surface of the sixth lens. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies 0.1≤ΣTP/InTL≤0.9, where InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens, and ΣTP is a sum of central thicknesses of the lenses on the optical axis. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system of the present invention satisfies 0.001≤|R1/R2|≤20, and a preferable range is 0.01≤|R1/R2|<10, where R1 is a radius of curvature of the object-side surface of the first lens, and R2 is a radius of curvature of the image-side surface of the first lens. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies −7<(R11−R12)/(R11+R12)<50, where R13 is a radius of curvature of the object-side surface of the seventh lens, and R14 is a radius of curvature of the image-side surface of the seventh lens. It may modify the astigmatic field curvature.

The optical image capturing system of the present invention satisfies IN12/f≤3.0, where IN12 is a distance on the optical axis between the first lens and the second lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies IN67/f≤0.8, where IN67 is a distance on the optical axis between the sixth lens and the seventh lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP1+IN12)/TP2≤50, where TP1 is a central thickness of the first lens on the optical axis, and TP2 is a central thickness of the second lens on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤(TP7+IN67)/TP6≤10, where TP6 is a central thickness of the sixth lens on the optical axis, TP7 is a central thickness of the seventh lens on the optical axis, and N67 is a distance between the sixth lens and the seventh lens. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≤TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the third lens on the optical axis, TP4 is a central thickness of the fourth lens on the optical axis, TP5 is a central thickness of the fifth lens on the optical axis, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens. It may fine tune and correct the aberration of the incident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≤HVT71≤3 mm; 0 mm<HVT72≤6 mm; 0≤HVT71/HVT72; 0 mm≤|SGC71|≤0.5 mm; 0 mm<|SGC72|≤2 mm; and 0<|SGC72|/(|SGC72|+TP7)≤0.9, where HVT71 a distance perpendicular to the optical axis between the critical point C71 on the object-side surface of the seventh lens and the optical axis; HVT72 a distance perpendicular to the optical axis between the critical point C72 on the image-side surface of the seventh lens and the optical axis; SGC71 is a distance on the optical axis between a point on the object-side surface of the seventh lens where the optical axis passes through and a point where the critical point C71 projects on the optical axis; SGC72 is a distance on the optical axis between a point on the image-side surface of the seventh lens where the optical axis passes through and a point where the critical point C72 projects on the optical axis. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≤HVT72/HOI≤0.9, and preferably satisfies 0.3≤HVT72/HOI≤0.8. It may help to correct the peripheral aberration.

The optical image capturing system satisfies 0≤HVT72/HOS≤0.5, and preferably satisfies 0.2≤HVT72/HOS≤0.45. It may help to correct the peripheral aberration.

The optical image capturing system of the present invention satisfies 0<SGI711/(SGI711+TP7)≤0.9; 0<SGI721/(SGI721+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI711/(SGI711+TP7)≤0.6; 0.1≤SGI721/(SGI721+TP7)≤0.6, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0<SGC712/(SGI712+TP7)≤0.9; 0≤SGI722/(SGI722+TP7)≤0.9, and it is preferable to satisfy 0.1≤SGI712/(SGI712+TP7)≤0.6; 0.1≤SGI722/(SGI722+TP7)≤0.6, where SGI712 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI722 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF711|≤5 mm; 0.001 mm≤|HIF721|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF711|≤3.5 mm; 1.5 mm≤|HIF721|≤3.5 mm, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF712|≤5 mm; 0.001 mm≤|HIF722|≤55 mm, and it is preferable to satisfy 0.1 mm≤|HIF722|≤3.5 mm; 0.1 mm|≤HIF712|≤0.5 mm, where HIF712 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis; HIF722 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤HIF713|≤5 mm; 0.001 mm≤|HIF723|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF723|≤3.5 mm; 0.1 mm≤|HIF713|≤3.5 mm, where HIF713 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis; HIF723 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≤|HIF714|≤5 mm; 0.001 mm≤|HIF724|≤5 mm, and it is preferable to satisfy 0.1 mm≤|HIF724|≤3.5 mm; 0.1 mm≤|HIF714|≤3.5 mm, where HIF714 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis; HIF724 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of low Abbe number are arranged in an interlaced arrangement that could be helpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ²/[1+[1(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹² +A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1)

where z is a depression of the aspheric surface; k is conic constant; c is reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made of plastic or glass. The plastic lenses may reduce the weight and lower the cost of the system, and the glass lenses may control the thermal effect and enlarge the space for arrangement of the refractive power of the system. In addition, the opposite surfaces (object-side surface and image-side surface) of the first to the seventh lenses could be aspheric that can obtain more control parameters to reduce aberration. The number of aspheric glass lenses could be less than the conventional spherical glass lenses, which is helpful for reduction of the height of the system.

When the lens has a convex surface, which means that the surface is convex around a position, through which the optical axis passes, and when the lens has a concave surface, which means that the surface is concave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could be applied in a dynamic focusing optical system. It is superior in the correction of aberration and high imaging quality so that it could be allied in lots of fields.

The optical image capturing system of the present invention could further include a driving module to meet different demands, wherein the driving module can be coupled with the lenses to move the lenses. The driving module can be a voice coil motor (VCM), which is used to move the lens for focusing, or can be an optical image stabilization (OIS) component, which is used to lower the possibility of having the problem of image blurring which is caused by subtle movements of the lens while shooting.

To meet different requirements, at least one lens among the first lens to the seventh lens of the optical image capturing system of the present invention can be a light filter, which filters out light of wavelength shorter than 500 nm. Such effect can be achieved by coating on at least one surface of the lens, or by using materials capable of filtering out short waves to make the lens.

To meet different requirements, the image plane of the optical image capturing system in the present invention can be either flat or curved. If the image plane is curved (e.g., a sphere with a radius of curvature), the incidence angle required for focusing light on the image plane can be decreased, which is not only helpful to shorten the length of the system (TTL), but also helpful to increase the relative illuminance.

We provide several embodiments in conjunction with the accompanying drawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 of the first embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 110, a second lens 120, a third lens 130, an aperture 100, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter 180, an image plane 190, and an image sensor 192. FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system 10 of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of the aperture 100. FIG. 1D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present invention. FIG. 1E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the first embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 110 has negative refractive power and is made of plastic. An object-side surface 112 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 114 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 112 has an inflection point thereon, and the image-side surface 114 has two inflection points. A profile curve length of the maximum effective half diameter of an object-side surface of the first lens 110 is denoted by ARS11, and a profile curve length of the maximum effective half diameter of the image-side surface of the first lens 10 is denoted by ARS12. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the first lens 110 is denoted by ARE11, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens 110 is denoted by ARE12. A thickness of the first lens 110 on the optical axis is TP1.

The first lens satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437, where SGI111 is a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI121 is a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The first lens satisfies SGI112=0 mm; SGI122=4.2315 mm; |SGI121|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where SGI112 is a displacement on the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI121 is a displacement on the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the second closest to the optical axis, projects on the optical axis.

The first lens satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127; HIF121=7.1744 mm; HIF121/HOI=0.9567, where HIF111 is a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis; HIF121 is a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis.

The first lens satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm; HIF122/HOI=1.3147, where HIF112 is a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis; HIF122 is a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis.

The second lens 120 has positive refractive power and is made of plastic. An object-side surface 122 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 124 thereof, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the second lens 120 is denoted by ARS21, and a profile curve length of the maximum effective half diameter of the image-side surface of the second lens 120 is denoted by ARS22. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the second lens 120 is denoted by ARE21, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens 120 is denoted by ARE22. A thickness of the second lens 120 on the optical axis is TP2.

For the second lens, a displacement on the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis, is denoted by SGI211, and a displacement on the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF211, and a displacement perpendicular to the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic. An object-side surface 132, which faces the object side, is a convex aspheric surface, and an image-side surface 134, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the third lens 130 is denoted by ARS31, and a profile curve length of the maximum effective half diameter of the image-side surface of the third lens 130 is denoted by ARS32. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the third lens 130 is denoted by ARE31, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the third lens 130 is denoted by ARE32. A thickness of the third lens 130 on the optical axis is TP3.

For the third lens 130, SGI311 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI321 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the third lens 130, SGI312 is a displacement on the optical axis from a point on the object-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI322 is a displacement on the optical axis from a point on the image-side surface of the third lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the closest to the optical axis, and the optical axis; HIF321 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the second closest to the optical axis, and the optical axis; HIF322 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the second closest to the optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made of plastic. An object-side surface 142, which faces the object side, is a convex aspheric surface, and an image-side surface 144, which faces the image side, is a convex aspheric surface. The object-side surface 142 has an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fourth lens 140 is denoted by ARS41, and a profile curve length of the maximum effective half diameter of the image-side surface of the fourth lens 140 is denoted by ARS42. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fourth lens 140 is denoted by ARE41, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fourth lens 140 is denoted by ARE42. A thickness of the fourth lens 140 on the optical axis is TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm; |SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI421 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fourth lens 140, SGI412 is a displacement on the optical axis from a point on the object-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI422 is a displacement on the optical axis from a point on the image-side surface of the fourth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm; HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis; HIF421 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis; HIF422 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic. An object-side surface 152, which faces the object side, is a concave aspheric surface, and an image-side surface 154, which faces the image side, is a convex aspheric surface. The object-side surface 152 and the image-side surface 154 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fifth lens 150 is denoted by ARS51, and a profile curve length of the maximum effective half diameter of the image-side surface of the fifth lens 150 is denoted by ARS52. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fifth lens 150 is denoted by ARE51, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fifth lens 150 is denoted by ARE52. A thickness of the fifth lens 50 on the optical axis is TP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm; |SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, where SGI511 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI521 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

For the fifth lens 150, SGI512 is a displacement on the optical axis from a point on the object-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis, and SGI522 is a displacement on the optical axis from a point on the image-side surface of the fifth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the second closest to the optical axis, projects on the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm; HIF511/HOI=0.5091, HIF521/HOI=0.6065, where HIF511 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis; HIF521 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis; HIF522 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis.

The sixth lens 160 has negative refractive power and is made of plastic. An object-side surface 162, which faces the object side, is a convex surface, and an image-side surface 164, which faces the image side, is a concave surface. The object-side surface 162 and the image-side surface 164 both have an inflection point, which could adjust the incident angle of each view field to improve aberration. A profile curve length of the maximum effective half diameter of an object-side surface of the sixth lens 160 is denoted by ARS61, and a profile curve length of the maximum effective half diameter of the image-side surface of the sixth lens 160 is denoted by ARS62. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the sixth lens 160 is denoted by ARE61, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the sixth lens 160 is denoted by ARE62. A thickness of the sixth lens 160 on the optical axis is TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm; |SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, where SGI611 is a displacement on the optical axis from a point on the object-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI621 is a displacement on the optical axis from a point on the image-side surface of the sixth lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm; HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis; HIF621 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis.

The seventh lens 170 has positive refractive power and is made of plastic. An object-side surface 172, which faces the object side, is a convex surface, and an image-side surface 174, which faces the image side, is a concave surface. This would help to shorten the back focal length, whereby to keep the optical image capturing system miniaturized. The object-side surface 172 and the image-side surface 174 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the seventh lens 170 is denoted by ARS71, and a profile curve length of the maximum effective half diameter of the image-side surface of the seventh lens 170 is denoted by ARS72. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the seventh lens 170 is denoted by ARE71, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the seventh lens 170 is denoted by ARE72. A thickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm; |SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, where SGI711 is a displacement on the optical axis from a point on the object-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the object-side surface, which is the closest to the optical axis, projects on the optical axis, and SGI721 is a displacement on the optical axis from a point on the image-side surface of the seventh lens, through which the optical axis passes, to a point where the inflection point on the image-side surface, which is the closest to the optical axis, projects on the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616 mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The infrared rays filter 180 is made of glass and between the seventh lens 170 and the image plane 190. The infrared rays filter 180 gives no contribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has the following parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968 deg; and tan(HAF)=1.7318, where f is a focal length of the system; HAF is a half of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm; |f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is a focal length of the first lens 110; and f7 is a focal length of the seventh lens 170.

The first embodiment further satisfies |f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and |f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of the second lens 120, f3 is a focal length of the third lens 130, f4 is a focal length of the fourth lens 140, f5 is a focal length of the fifth lens 150, and f6 is a focal length of the sixth lens 160.

The optical image capturing system 10 of the first embodiment further satisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999; ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411; |f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=7.5187, where PPR is a ratio of a focal length fp of the optical image capturing system to a focal length fp of each of the lenses with positive refractive power, and NPR is a ratio of a focal length fn of the optical image capturing system to a focal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment further satisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977; HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170; HOS is a height of the image capturing system, i.e. a distance between the object-side surface 112 of the first lens 110 and the image plane 190; InS is a distance between the aperture 100 and the image plane 190; HOI is a half of a diagonal of an effective sensing area of the image sensor 192, i.e., the maximum image height; and BFL is a distance between the image-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment further satisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of the thicknesses of the lenses 110-150 with refractive power. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment further satisfies |R1/R2|=129.9952, where R1 is a radius of curvature of the object-side surface 112 of the first lens 110, and R2 is a radius of curvature of the image-side surface 114 of the first lens 110. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment further satisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius of curvature of the object-side surface 172 of the seventh lens 170, and R14 is a radius of curvature of the image-side surface 174 of the seventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment further satisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, where ΣPP is a sum of the focal length fp of each lens with positive refractive power. It is helpful to share the positive refractive power of the fourth lens 140 to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNP is a sum of the focal length fn of each lens with negative refractive power. It is helpful to share the negative refractive power of the first lens 110 to other negative lenses, which avoids the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on the optical axis between the first lens 110 and the second lens 120. It may correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, where TP1 is a central thickness of the first lens 110 on the optical axis, and TP2 is a central thickness of the second lens 120 on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, where TP6 is a central thickness of the sixth lens 160 on the optical axis, TP7 is a central thickness of the seventh lens 170 on the optical axis, and IN67 is a distance on the optical axis between the sixth lens 160 and the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm; IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a central thickness of the third lens 130 on the optical axis, TP4 is a central thickness of the fourth lens 140 on the optical axis, TP5 is a central thickness of the fifth lens 150 on the optical axis, IN34 is a distance on the optical axis between the third lens 130 and the fourth lens 140, IN45 is a distance on the optical axis between the fourth lens 140 and the fifth lens 150, and InTL is a distance from the object-side surface 112 of the first lens 110 to the image-side surface 174 of the seventh lens 170 on the optical axis. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6=0.722, where InRS61 is a displacement from a point on the object-side surface 162 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 162 of the sixth lens 160 ends; InRS62 is a displacement from a point on the image-side surface 166 of the sixth lens 160 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 166 of the sixth lens 160 ends; and TP6 is a central thickness of the sixth lens 160 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment further satisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404, where HVT61 is a distance perpendicular to the optical axis between the critical point on the object-side surface 162 of the sixth lens and the optical axis; and HVT62 is a distance perpendicular to the optical axis between the critical point on the image-side surface 166 of the sixth lens and the optical axis.

The optical image capturing system 10 of the first embodiment further satisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm, and |InRS72|/TP7=0.0839, where InRS71 is a displacement from a point on the object-side surface 172 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the object-side surface 172 of the seventh lens 170 ends; InRS72 is a displacement from a point on the image-side surface 174 of the seventh lens 170 passed through by the optical axis to a point on the optical axis where a projection of the maximum effective semi diameter of the image-side surface 174 of the seventh lens 170 ends; and TP7 is a central thickness of the seventh lens 170 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfies HVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 a distance perpendicular to the optical axis between the critical point on the object-side surface 172 of the seventh lens and the optical axis; and HVT72 a distance perpendicular to the optical axis between the critical point on the image-side surface 174 of the seventh lens and the optical axis.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOI=0.5414. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOS=0.1505. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment further satisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; and ODT is optical distortion.

In the present embodiment, the lights of any field of view can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. The focus shifts where the through-focus MTF values of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima are denoted by VSFS0, VSFS3, and VSFS7 (unit of measurement: mm), respectively. The values of VSFS0, VSFS3, and VSFS7 equal to −0.010 mm, −0.005 mm, and −0.015 mm, respectively. The maximum values of the through-focus MTF of the visible sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VSMTF0, VSMTF3, and VSMTF7, respectively. The values of VSMTF0, VSMTF3, and VSMTF7 equal to 0.891, 0.898, and 0.892, respectively. The focus shifts where the through-focus MTF values of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by VTFS0, VTFS3, and VTFS7 (unit of measurement: mm), respectively. The values of VTFS0, VTFS3, and VTFS7 equal to −0.010 mm, −0.015 mm, and −0.025 mm, respectively. The maximum values of the through-focus MTF of the visible tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by VTMTF0, VTMTF3, and VTMTF7, respectively. The values of VTMTF0, VTMTF3, and VTMTF7 equal to 0.891, 0.272, and 0.251, respectively. The average focus shift (position) of both the aforementioned focus shifts of the visible sagittal ray at three fields of view and focus shifts of the visible tangential ray at three fields of view is denoted by AVFS (unit of measurement: mm), which satisfies the absolute value |(VSFS0+VSFS3+VSFS7+VTFS0+VTFS3+VTFS7)/6|=|−0.008 mm|.

The focus shifts where the through-focus MTF values of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ISFS0, ISFS3, and ISFS7 (unit of measurement: mm), respectively. The values of ISFS0, ISFS3, and ISFS7 equal to −0.005 mm, −0.005 mm, and 0.015 mm, respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared sagittal ray at three fields of view is denoted by AISFS (unit of measurement: mm). The maximum values of the through-focus MTF of the infrared sagittal ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ISMTF0, ISMTF3, and ISMTF7, respectively. The values of ISMTF0, ISMTF3, and ISMTF7 equal to 0.868, 0.869, and 0.846, respectively. The focus shifts where the through-focus MTF values of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view of the optical image capturing system are at their respective maxima, are denoted by ITFS0, ITFS3, and ITFS7 (unit of measurement: mm), respectively. The values of ITFS0, ITFS3, and ITFS7 equal to −0.005, −0.010, and 0.015, respectively. The average focus shift (position) of the aforementioned focus shifts of the infrared tangential ray at three fields of view is denoted by AITFS (unit of measurement: mm). The maximum values of the through-focus MTF of the infrared tangential ray at the central field of view, 0.3 field of view, and 0.7 field of view are denoted by ITMTF0, ITMTF3, and ITMTF7, respectively. The values of ITMTF0, ITMTF3, and ITMTF7 equal to 0.868, 0.870, and 0.828, respectively. The average focus shift (position) of both of the aforementioned focus shifts of the infrared sagittal ray at the three fields of view and focus shifts of the infrared tangential ray at the three fields of view is denoted by AIFS (unit of measurement: mm), which equals to the absolute value of |(ISFS0+ISFS3+ISFS7+ITFS0+ITFS3+ITFS7)/6|=−0.004 mm|.

The focus shift (difference) between the focal points of the visible light and the infrared light at their central fields of view (RGB/IR) of the entire optical image capturing system (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm) is denoted by FS (the distance between the first and second image planes on the optical axis), which satisfies the absolute value |(VSFS0+VTFS0)/2−(ISFS0+ITFS0)/2|=|0.005 mm|. The difference (focus shift) between the average focus shift of the visible light in the three fields of view and the average focus shift of the infrared light in the three fields of view (RGB/IR) of the entire optical image capturing system is denoted by AFS (i.e. wavelength of 850 nm versus wavelength of 555 nm, unit of measurement: mm), for which the absolute value of |AIFS−AVFS|=|0.004 mm| is satisfied.

In the optical image capturing system 10 of the first embodiment, a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PSTA, and is 0.00040 mm; a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PLTA, and is −0.009 mm a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NSTA, and is −0.002 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NLTA, and is −0.016 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SSTA, and is 0.018 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SLTA, and is 0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table 1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens −1079.499964 2.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens 14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd) lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7 Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.00 9.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic 1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.8673642751 0.300 plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens 1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Image plane plane Reference wavelength: 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01 −2.915013E+00 4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−05  4.353586E−04  5.793768E−04 −3.756697E−04  −1.292614E−03 A6 −3.014384E−08  −1.838670E−06 2.334364E−06  1.400287E−05  2.112652E−04 3.901218E−04 −1.602381E−05 A8 −2.487400E−10   9.605910E−09 −7.479362E−08  −1.688929E−07 −1.344586E−05 −4.925422E−05  −8.452359E−06 A10 1.170000E−12 −8.256000E−11 1.701570E−09  3.829807E−08  1.000482E−06 4.139741E−06  7.243999E−07 A12 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00  −5.000000E+01 −1.740728E+00  −4.709650E+00 −4.509781E+00 −3.427137E+00  −3.215123E+00 A4 −5.583548E−03   1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03  −2.815022E−03 A6 1.947110E−04 −4.949077E−05 −4.981838E−05  −1.523141E−05 −2.688331E−05 −1.058126E−05   1.884580E−05 A8 −1.486947E−05   2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07 1.760103E−06 −1.017223E−08 A10 −6.501246E−08  −1.438383E−08 7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08   3.660000E−12 A12 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 A14 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00

The figures related to the profile curve lengths obtained based on Table 1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.792 1.792 −0.00044 99.98% 2.276 78.73% 12 1.792 1.806 0.01319 100.74% 2.276 79.33% 21 1.792 1.797 0.00437 100.24% 5.240 34.29% 22 1.792 1.792 −0.00032 99.98% 5.240 34.20% 31 1.792 1.808 0.01525 100.85% 0.837 216.01% 32 1.792 1.819 0.02705 101.51% 0.837 217.42% 41 1.792 1.792 −0.00041 99.98% 2.002 89.50% 42 1.792 1.825 0.03287 101.83% 2.002 91.16% 51 1.792 1.792 −0.00031 99.98% 4.271 41.96% 52 1.792 1.845 0.05305 102.96% 4.271 43.21% 61 1.792 1.818 0.02587 101.44% 0.300 606.10% 62 1.792 1.874 0.08157 104.55% 0.300 624.67% 71 1.792 1.898 0.10523 105.87% 1.118 169.71% 72 1.792 1.885 0.09273 105.17% 1.118 168.59% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 15.095 15.096 0.001 100.01% 2.276 663.24% 12 10.315 11.377 1.062 110.29% 2.276 499.86% 21 7.531 8.696 1.166 115.48% 5.240 165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.632 4.013 0.382 110.51% 0.837 479.55% 32 2.815 3.159 0.344 112.23% 0.837 377.47% 41 2.967 2.971 0.004 100.13% 2.002 148.38% 42 3.402 3.828 0.426 112.53% 2.002 191.20% 51 4.519 4.523 0.004 100.10% 4.271 105.91% 52 5.016 5.722 0.706 114.08% 4.271 133.99% 61 5.019 5.823 0.805 116.04% 0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.300 2201.71% 71 5.634 6.503 0.869 115.43% 1.118 581.54% 72 6.488 7.152 0.664 110.24% 1.118 639.59%

The detail parameters of the first embodiment are listed in Table 1, in which the unit of the radius of curvature, thickness, and focal length are millimeter, and surface 0-10 indicates the surfaces of all elements in the system in sequence from the object side to the image side. Table 2 is the list of coefficients of the aspheric surfaces, in which A1-A20 indicate the coefficients of aspheric surfaces from the first order to the twentieth order of each aspheric surface. The following embodiments have the similar diagrams and tables, which are the same as those of the first embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 of the second embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 210, a second lens 220, an aperture 200, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seventh lens 270, an infrared rays filter 280, an image plane 290, and an image sensor 292. FIG. 2C shows a transverse aberration diagram at 0.7 field of view of the second embodiment of the present invention. FIG. 2D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present invention. FIG. 2E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the second embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 210 has negative refractive power and is made of glass. An object-side surface 212 thereof, which faces the object side, is a convex spherical surface, and an image-side surface 214 thereof, which faces the image side, is a concave spherical surface.

The second lens 220 has negative refractive power and is made of glass. An object-side surface 222 thereof, which faces the object side, is a convex spherical surface, and an image-side surface 224 thereof, which faces the image side, is a concave spherical surface.

The third lens 230 has positive refractive power and is made of glass. An object-side surface 232, which faces the object side, is a concave spherical surface, and an image-side surface 234, which faces the image side, is a convex spherical surface. The object-side surface 232 has an inflection point

The fourth lens 240 has positive refractive power and is made of glass. An object-side surface 242, which faces the object side, is a convex spherical surface, and an image-side surface 244, which faces the image side, is a convex spherical surface.

The fifth lens 250 has positive refractive power and is made of glass. An object-side surface 252, which faces the object side, is a convex spherical surface, and an image-side surface 254, which faces the image side, is a convex spherical surface.

The sixth lens 260 has negative refractive power and is made of glass. An object-side surface 262, which faces the object side, is a concave spherical surface, and an image-side surface 264, which faces the image side, is a convex spherical surface. Whereby, the incident angle of each view field could be adjusted to improve aberration.

The seventh lens 270 has positive refractive power and is made of glass. An object-side surface 272, which faces the object side, is a convex spherical surface, and an image-side surface 274, which faces the image side, is a concave spherical surface. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventh lens 270 and the image plane 290. The infrared rays filter 280 gives no contribution to the focal length of the system.

The parameters of the lenses of the second embodiment are listed in Table 3 and Table 4.

TABLE 3 f = 1.1063 mm; f/HEP = 1.2; HAF = 100 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 12.81416352 2.000 glass 2.001 29.13 −5.48966 2 3.560026641 3.032 3 2^(nd) lens 10.67329511 2.000 glass 2.001 29.13 −3.67309 4 2.488957865 4.704 5 Aperture 1E+18 0.203 6 3^(rd) lens −346.5103482 2.299 glass 1.497 81.56 10.5734 7 −5.209502519 0.200 8 4^(th) lens 11.84741378 2.404 glass 1.497 81.56 11.7876 9 −10.85986117 0.200 10 5^(th) lens 6.243441203 2.753 glass 1.497 81.56 7.96561 11 −9.295107665 0.306 12 6^(th) lens −6.585154258 2.000 glass 2.002 19.32 −8.96126 13 −27.79175646 0.200 14 7^(th) lens 6.278931408 2.474 glass 1.658 50.85 10.0301 15 100.5655695 0.224 16 Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.003 18 Image 1E+18 −0.003 plane Reference wavelength: 555 nm; the position of blocking light: the effective half diameter of the clear aperture of the fourth surface is 2.150 mm; the effective diameter of the clear aperture of the seventh surface is 1.750 mm.

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the second embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.2015 0.3012 0.1046 0.0938 0.1389 0.1234 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1103 0.5234 0.5503 0.9511 2.7410 0.1808 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 1.4946 0.3474 2.5161 1.3370 HOS InTL HOS/HOI InS/HOS ODT % TDT % 26.9997 24.7763 14.8841 0.5653 −129.0830 90.6623 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTA NSTA NLTA SSTA SLTA −0.022 mm 0.018 mm −0.025 mm 0.021 mm 0.005 mm 0.001 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.010 −0.005 0.015 −0.010 −0.015 −0.025 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.891 0.898 0.892 0.891 0.272 0.251 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 −0.005 −0.005 0.015 −0.005 −0.010 −0.015 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.868 0.869 0.846 0.868 0.870 0.828 FS AIFS AVFS AFS 0.005 −0.004 −0.008 0.004

The figures related to the profile curve lengths obtained based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP 11 0.461 0.460 −0.00084 99.82% 2.000 23.00% 12 0.461 0.461 0.00035 100.08% 2.000 23.06% 21 0.461 0.460 −0.00080 99.83% 2.000 23.01% 22 0.461 0.463 0.00172 100.37% 2.000 23.13% 31 0.461 0.460 −0.00094 99.80% 2.299 20.00% 32 0.461 0.461 −0.00034 99.93% 2.299 20.03% 41 0.461 0.460 −0.00082 99.82% 2.404 19.14% 42 0.461 0.460 −0.00080 99.83% 2.404 19.14% 51 0.461 0.460 −0.00052 99.89% 2.753 16.72% 52 0.461 0.460 −0.00075 99.84% 2.753 16.71% 61 0.461 0.460 −0.00056 99.88% 2.000 23.02% 62 0.461 0.460 −0.00092 99.80% 2.000 23.00% 71 0.461 0.460 −0.00053 99.89% 2.474 18.61% 72 0.461 0.460 −0.00094 99.80% 2.474 18.59% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 8.511 9.307 0.79639 109.36% 2.000 465.35% 12 3.553 5.368 1.81526 151.09% 2.000 268.42% 21 3.330 3.385 0.05576 101.67% 2.000 169.27% 22 2.150 2.593 0.44349 120.63% 2.000 129.67% 31 1.393 1.392 −0.00079 99.94% 2.299 60.54% 32 1.750 1.785 0.03483 101.99% 2.299 77.62% 41 1.965 1.974 0.00866 100.44% 2.404 82.11% 42 2.271 2.288 0.01650 100.73% 2.404 95.16% 51 2.384 2.445 0.06133 102.57% 2.753 88.80% 52 2.269 2.291 0.02214 100.98% 2.753 83.21% 61 2.225 2.269 0.04399 101.98% 2.000 113.43% 62 2.399 2.401 0.00243 100.10% 2.000 120.05% 71 2.451 2.518 0.06678 102.72% 2.474 101.77% 72 2.196 2.196 −0.00010 100.00% 2.474 88.77%

The results of the equations of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment (Reference wavelength: 555 nm) HIF311 0 HIF311/HOI 0 SGI311 0 |SGI311|/ 0 (|SGI311| + TP3)

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system of the third embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 310, a second lens 320, an aperture 300, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter 380, an image plane 390, and an image sensor 392. FIG. 3C shows a transverse aberration diagram at 0.7 field of view of the third embodiment of the present invention. FIG. 3D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present invention. FIG. 3E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the third embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 310 has negative refractive power and is made of glass. An object-side surface 312 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 314 thereof, which faces the image side, is a concave aspheric surface.

The second lens 320 has positive refractive power and is made of glass. An object-side surface 322 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 324 thereof, which faces the image side, is a convex aspheric surface.

The third lens 330 has negative refractive power and is made of glass. An object-side surface 332 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 334 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 322 has an inflection point, and the image-side surface 334 has an inflection point.

The fourth lens 340 has positive refractive power and is made of glass. An object-side surface 342, which faces the object side, is a convex aspheric surface, and an image-side surface 344, which faces the image side, is a convex aspheric surface. The object-side surface 342 has an inflection point.

The fifth lens 350 has positive refractive power and is made of plastic. An object-side surface 352, which faces the object side, is a convex aspheric surface, and an image-side surface 354, which faces the image side, is a convex aspheric surface. The object-side surface 352 has an inflection point. It may help to shorten the back focal length to keep small in size.

The sixth lens 360 has positive refractive power and is made of glass. An object-side surface 362, which faces the object side, is a convex aspheric surface, and an image-side surface 364, which faces the image side, is a convex aspheric surface. The object-side surface 362 has an inflection point, and the image-side surface 364 has an inflection point. Whereby, the incident angle of each view field could be adjusted to improve aberration.

The seventh lens 370 has negative refractive power and is made of glass. An object-side surface 372, which faces the object side, is a concave aspheric surface, and an image-side surface 374, which faces the image side, is a convex aspheric surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 372 has an inflection point, and the image-side surface 374 has two inflection points, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventh lens 370 and the image plane 390. The infrared rays filter 380 gives no contribution to the focal length of the system.

The parameters of the lenses of the third embodiment are listed in Table 5 and Table 6.

TABLE 5 f = 3.2527 mm; f/HEP = 1.6; HAF = 100 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 18.43462476 2.000 glass 2.001 29.13 −8.91581 2 5.709746751 6.239 3 2^(nd) lens −13.23328183 9.571 glass 2.002 19.32 15.0427 4 −9.648795938 1.858 5 Aperture 1E+18 0.436 6 3^(rd) lens 85.04549784 2.000 glass 2.002 19.32 −14.5159 7 12.36748049 0.267 8 4^(th) lens 28.73730258 4.161 glass 1.497 81.56 11.6676 9 −6.936276207 0.200 10 5^(th) lens 17.69746786 3.116 glass 1.497 81.56 30.3273 11 −97.287663 0.200 12 6^(th) lens 7.610112562 5.214 glass 1.497 81.56 8.86673 13 −8.13132248 0.321 14 7^(th) lens −6.470602521 2.000 glass 2.002 19.32 −8.27735 15 −32.96956359 0.418 16 Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.000 18 Image 1E+18 0.006 plane Reference wavelength: 555 nm; the position of blocking light: the effective half diameter of the clear aperture of the ninth surface is 4.500 mm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 7.833779E−05 −1.102508E−04  −1.195991E−04  5.750004E−04 −5.966606E−04  −6.114253E−04  1.830109E−03 A6 −3.778056E−07  −9.764729E−07  1.366886E−05 −8.640009E−06  −3.553601E−05  −4.853131E−06  −8.189844E−05  A8 0.000000E+00 1.977155E−17 −4.888384E−07  1.649385E−07 3.991516E−06 −2.228917E−06  −1.774810E−06  A10 0.000000E+00 3.210507E−21 6.370354E−09 6.724570E−10 −1.907188E−07  5.707495E−08 1.376916E−08 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 6.583832E−04 −2.666867E−04  −7.163402E−04  −9.296122E−05  2.301903E−04 3.114617E−04 1.645779E−03 A6 −2.447085E−05  2.245654E−06 1.209701E−05 −2.728331E−06  −1.264738E−05  4.164839E−05 −9.329592E−05  A8 1.087688E−06 −3.335222E−07  1.111150E−07 −1.835631E−07  7.185962E−07 1.140767E−07 3.190350E−06 A10 −4.567453E−08  3.932960E−09 −6.999095E−09  −7.583020E−09  1.387767E−08 4.715151E−09 −4.470870E−08  A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the third embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.3648 0.2162 0.2241 0.2788 0.1073 0.3668 |f/f7| ΣPPR ΣNPR ΣPPR/ΣNPR| IN12/f IN67/f 0.3930 1.2345 0.7165 1.7231 1.9181 0.0986 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.5927 1.0363 0.8608 0.4451 HOS InTL HOS/HOI InS/HOS ODT % TDT % 39.9997 37.5825 7.9999 0.5083 −127.1830 106.6900 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 00000 0.0000 0.0000 2.0293 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 5.2141 5.2003 3.1075 0.6215 0.0777 PSTA PLTA NSTA NLTA SSTA SLTA −0.044 mm −0.029 mm −0.024 mm −0.004 mm 0.011 mm −0.013 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.010 −0.000 −0.020 0.010 0.015 0.010 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.721 0.663 0.064 0.721 0.421 0.629 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.010 −0.000 −0.030 0.010 0.015 0.020 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.560 0.499 0.600 0.560 0.413 0.499 FS AIFS AVFS AFS 0.000 0.004 0.004 0.000

The figures related to the profile curve lengths obtained based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.017 1.017 −0.00002 100.00% 2.000 50.83% 12 1.017 1.021 0.00488 100.48% 2.000 51.07% 21 1.017 1.017 0.00047 100.05% 9.571 10.63% 22 1.017 1.018 0.00129 100.13% 9.571 10.63% 31 1.017 1.016 −0.00052 99.95% 2.000 50.80% 32 1.017 1.017 0.00056 100.06% 2.000 50.86% 41 1.017 1.016 −0.00027 99.97% 4.161 24.43% 42 1.017 1.020 0.00305 100.30% 4.161 24.51% 51 1.017 1.017 0.00000 100.00% 3.116 32.62% 52 1.017 1.016 −0.00052 99.95% 3.116 32.61% 61 1.017 1.019 0.00249 100.24% 5.214 19.54% 62 1.017 1.019 0.00210 100.21% 5.214 19.54% 71 1.017 1.020 0.00363 100.36% 2.000 51.01% 72 1.017 1.016 −0.00042 99.96% 2.000 50.81% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 11.191 12.248 1.05713 109.45% 2.000 612.42% 12 5.665 8.137 2.47143 143.63% 2.000 406.83% 21 5.419 5.576 0.15666 102.89% 9.571 58.26% 22 4.642 4.768 0.12588 102.71% 9.571 49.82% 31 2.974 2.973 −0.00064 99.98% 2.000 148.66% 32 3.641 3.664 0.02342 100.64% 2.000 183.20% 41 3.808 3.826 0.01806 100.47% 4.161 91.97% 42 4.500 4.857 0.35727 107.94% 4.161 116.74% 51 5.322 5.351 0.02907 100.55% 3.116 171.73% 52 5.599 5.656 0.05706 101.02% 3.116 181.51% 61 5.646 6.025 0.37875 106.71% 5.214 115.56% 62 5.514 5.746 0.23170 104.20% 5.214 110.20% 71 5.537 5.781 0.24385 104.40% 2.000 289.06% 72 5.297 5.299 0.00124 100.02% 2.000 264.93%

The results of the equations of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment (Reference wavelength: 555 nm) HIF311 1.1923 HIF311/HOI 0.2385 SGI311 0.0071 |SGI311|/(|SGI311| + TP3) 0.0035 HIF321 2.6242 HIF321/HOI 0.5248 SGI321 0.2469 |SGI321|/(|SGI321| + TP3) 0.1099 HIF411 2.8684 HIF411/HOI 0.5737 SGI411 0.2142 |SGI411|/(|SGI411| + TP4) 0.0490 HIF511 3.5883 HIF511/HOI 0.7177 SGI511 0.3204 |SGI511|/(|SGI511| + TP5) 0.0932 HIF611 4.4782 HIF611/HOI 0.8956 SGI611 1.3434 |SGI611|/(|SGI611| + TP6) 0.2049 HIF621 3.9742 HIF621/HOI 0.7948 SGI621 −0.9714 |SGI621|/(|SGI621| + TP6) 0.1571 HIF711 3.5268 HIF711/HOI 0.7054 SGI711 −0.9132 |SGI711|/(|SGI711| + TP7) 0.3135 HIF721 1.4393 HIF721/HOI 0.2879 SGI721 −0.0251 |SGI721|/(|SGI721| + TP7) 0.0124 HIF722 4.7428 HIF722/HOI 0.9486 SGI722 −0.0127 |SGI722|/(|SGI722| + TP7) 0.0063

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 of the fourth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 410, a second lens 420, an aperture 400, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, an infrared rays filter 480, an image plane 490, and an image sensor 492. FIG. 4C shows a transverse aberration diagram at 0.7 field of view of the fourth embodiment of the present invention. FIG. 4D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present invention. FIG. 4E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fourth embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 410 has negative refractive power and is made of glass. An object-side surface 412 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 414 thereof, which faces the image side, is a concave aspheric surface.

The second lens 420 has positive refractive power and is made of glass. An object-side surface 422 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 424 thereof, which faces the image side, is a convex aspheric surface.

The third lens 430 has positive refractive power and is made of glass. An object-side surface 432 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 434 thereof, which faces the image side, is a convex aspheric surface.

The fourth lens 440 has negative refractive power and is made of glass. An object-side surface 442, which faces the object side, is a convex aspheric surface, and an image-side surface 444, which faces the image side, is a concave aspheric surface. The object-side surface 442 has an inflection point, and the image-side surface 444 has an inflection point.

The fifth lens 450 has positive refractive power and is made of glass. An object-side surface 452, which faces the object side, is a convex aspheric surface, and an image-side surface 454, which faces the image side, is a convex aspheric surface. The object-side surface 452 has an inflection point.

The sixth lens 460 has positive refractive power and is made of glass. An object-side surface 462, which faces the object side, is a convex aspheric surface, and an image-side surface 464, which faces the image side, is a convex aspheric surface. The object-side surface 462 has an inflection point, and the image-side surface 464 has an inflection point. Whereby, the incident angle of each view field could be adjusted to improve aberration.

The seventh lens 470 has positive refractive power and is made of glass. An object-side surface 472, which faces the object side, is a concave aspheric surface, and an image-side surface 474, which faces the image side, is a convex aspheric surface. The object-side surface 472 has an inflection point, and the image-side surface 474 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventh lens 470 and the image plane 490. The infrared rays filter 480 gives no contribution to the focal length of the system.

The parameters of the lenses of the fourth embodiment are listed in Table 7 and Table 8.

TABLE 7 f = 2.3139 mm; f/HEP = 1.8; HAF = 100 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 18.0425411 2.000 glass 2.001 29.13 −4.9146 2 3.668251896 3.518 3 2^(nd) lens −9.093475153 4.908 glass 2.002 19.32 8.61225 4 −5.654915667 0.200 5 Aperture 1E+18 0.517 glass 6 3^(rd) lens −4.253968136 2.733 1.497 81.56 23.509 7 −3.787186957 0.200 8 4^(th) lens 24.23869014 2.000 glass 2.002 19.32 −10.6702 9 7.155354174 0.217 10 5^(th) lens 8.765494987 4.469 glass 1.497 81.56 8.1515 11 −6.284490286 0.200 12 6^(th) lens 9.707626166 4.623 glass 1.497 81.56 8.21822 13 −5.959849574 0.197 14 7^(th) lens −5.982321796 2.000 glass 2.002 19.32 42.9897 15 −6.1423035 0.219 16 Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.002 18 Image 1E+18 −0.003 plane Reference wavelength: 555 nm; the position of blocking light: the effective half diameter of the clear aperture of the seventh surface is 5.500 mm; the effective diameter of the clear aperture of the eleventh surface is 5.750 mm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 3.628081E−04 −9.382537E−04  −6.182000E−04  3.090272E−03 8.126609E−03 −2.456014E−04  −3.856670E−03  A6 −1.848280E−06  8.644205E−05 4.255409E−05 −6.301403E−05  −7.405758E−04  3.161645E−06 2.517445E−05 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 −2.835953E−03  −2.643505E−05  9.523945E−04 1.030953E−03 4.361332E−04 1.871837E−03 5.921034E−03 A6 −1.384629E−05  −7.378358E−05  −1.586426E−05  −2.524249E−05  1.033616E−04 4.308778E−05 −7.362674E−05  A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fourth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.4708 0.2687 0.0984 0.2169 0.2839 0.2816 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.0538 1.0677 0.6064 1.7608 1.5203 0.0852 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.5707 0.3663 1.1242 0.4753 HOS InTL HOS/HOI InS/HOS ODT % TDT % 29.9998 27.7810 6.0000 0.6458 −138.3440 114.0070 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 4.2870 4.4553 3.1242 0.6248 0.1041 PSTA PLTA NSTA NLTA SSTA SLTA −0.022 mm 0.005 mm −0.014 mm 0.017 mm 0.012 mm −0.010 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 0.025 −0.015 −0.010 0.025 0.005 −0.015 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.886 0.812 0.784 0.886 0.281 0.433 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 0.025 −0.025 −0.030 0.025 0.010 0 015 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.825 0.829 0.795 0.825 0.635 0.687 FS AIFS AVFS AFS 0.000 0.003 0.003 0.000

The figures related to the profile curve lengths obtained based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARS − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 0.643 0.642 −0.00063 99.90% 2.000 32.11% 12 0.643 0.645 0.00254 100.39% 2.000 32.27% 21 0.643 0.643 −0.00023 99.96% 4.908 13.09% 22 0.643 0.643 0.00057 100.09% 4.908 13.11% 31 0.643 0.644 0.00154 100.24% 2.733 23.58% 32 0.643 0.645 0.00236 100.37% 2.733 23.61% 41 0.643 0.642 −0.00070 99.89% 2.000 32.10% 42 0.643 0.643 0.00006 100.01% 2.000 32.14% 51 0.643 0.643 −0.00019 99.97% 4.469 14.38% 52 0.643 0.643 0.00034 100.05% 4.469 14.39% 61 0.643 0.642 −0.00029 99.96% 4.623 13.90% 62 0.643 0.643 0.00048 100.07% 4.623 13.91% 71 0.643 0.643 0.00045 100.07% 2.000 32.16% 72 0.643 0.643 0.00033 100.05% 2.000 32.15% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 7.900 8.586 0.68629 108.69% 2.000 429.30% 12 3.531 4.782 1.25038 135.41% 2.000 239.08% 21 3.156 3.227 0.07064 102.24% 4.908 65.74% 22 2.364 2.412 0.04859 102.06% 4.908 49.15% 31 1.735 1.772 0.03633 102.09% 2.733 64.83% 32 2.500 2.735 0.23513 109.41% 2.733 100.09% 41 2.890 2.898 0.00756 100.26% 2.000 144.88% 42 3.656 3.691 0.03545 100.97% 2.000 184.56% 51 3.932 3.996 0.06453 101.64% 4.469 89.42% 52 5.750 6.960 1.21039 121.05% 4.469 155.75% 61 5.163 5.544 0.38168 107.39% 4.623 119.93% 62 4.910 5.085 0.17516 103.57% 4.623 110.00% 71 4.924 5.040 0.11617 102.36% 2.000 252.02% 72 4.748 4.802 0.05420 101.14% 2.000 240.12%

The results of the equations of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment (Reference wavelength: 555 nm) HIF411 0.9523 HIF411/HOI 0.1905 SGI411 0.0156 |SGI411|/(|SGI411| + TP4) 0.0077 HIF421 2.1131 HIF421/HOI 0.4226 SGI421 0.2614 |SGI421|/(|SGI421| + TP4) 0.1156 HIF511 2.7747 HIF511/HOI 0.5549 SGI511 0.4155 |SGI511|/(|SGI511| + TP5) 0.0851 HIF611 4.9979 HIF611/HOI 0.9996 SGI611 1.6353 |SGI611|/(|SGI611| + TP6) 0.2613 HIF621 2.8526 HIF621/HOI 0.5705 SGI621 −0.6424 |SGI621|/(|SGI621| + TP6) 0.1220 HIF711 2.7179 HIF711/HOI 0.5436 SGI711 −0.5335 |SGI711|/(|SGI711| + TP7) 0.2106 HIF721 1.6799 HIF721/HOI 0.3360 SGI721 −0.1887 |SGI721|/(|SGI721| + TP7) 0.0862 HIF722 4.5290 HIF722/HOI 0.9058 SGI722 −0.1373 |SGI722|/(|SGI722| + TP7) 0.0642

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system of the fifth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 510, a second lens 520, an aperture 500, a third lens 530, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter 580, an image plane 590, and an image sensor 592. FIG. 5C shows a transverse aberration diagram at 0.7 field of view of the fifth embodiment of the present invention. FIG. 5D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present invention. FIG. 5E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the fifth embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 510 has negative refractive power and is made of glass. An object-side surface 512, which faces the object side, is a convex spherical surface, and an image-side surface 514, which faces the image side, is a concave spherical surface.

The second lens 520 has positive refractive power and is made of glass. An object-side surface 522 thereof, which faces the object side, is a concave spherical surface, and an image-side surface 524 thereof, which faces the image side, is a convex spherical surface.

The third lens 530 has positive refractive power and is made of glass. An object-side surface 532, which faces the object side, is a convex spherical surface, and an image-side surface 534, which faces the image side, is a convex spherical surface.

The fourth lens 540 has negative refractive power and is made of glass. An object-side surface 542, which faces the object side, is a concave spherical surface, and an image-side surface 544, which faces the image side, is a convex spherical surface.

The filth lens 550 has positive refractive power and is made of glass. An object-side surface 552, which faces the object side, is a convex spherical surface, and an image-side surface 554, which faces the image side, is a convex spherical surface.

The sixth lens 560 has positive refractive power and is made of glass. An object-side surface 562, which faces the object side, is a convex spherical surface, and an image-side surface 564, which faces the image side, is a concave spherical surface. Whereby, the incident angle of each view field could be adjusted to improve aberration.

The seventh lens 570 has negative refractive power and is made of glass. An object-side surface 572, which faces the object side, is a concave surface, and an image-side surface 574, which faces the image side, is a convex surface. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 570 is made of glass and between the seventh lens 570 and the image plane 590. The infrared rays filter 570 gives no contribution to the focal length of the system.

The parameters of the lenses of the fifth embodiment are listed in Table 9 and Table 10.

TABLE 9 f = 3.5977 mm; f/HEP = 1.8; HAF = 80 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 16.3941175 4.582 glass 2.001 29.13 −6.41877 2 3.986360017 4.318 3 2^(nd) lens −22.36861656 8.000 glass 2.002 19.32 15.9169 4 −11.04161103 0.340 5 Aperture 1E+18 1.912 glass 6 3^(rd) lens 18.0888417 3.663 1.497 81.56 8.53923 7 −5.188198284 0.267 8 4^(th) lens −5.023943006 2.000 glass 2.002 19.32 −11.5176 9 −10.60513926 0.200 10 5^(th) lens 66.93373932 3.890 glass 1.497 81.56 16.8097 11 −9.387754651 0.200 12 6^(th) lens 9.397825843 3.646 glass 1.694 53.20 15.6298 13 58.12299156 1.271 14 7^(th) lens −15.41329257 2.000 glass 2.002 19.32 −16.6095 15 −200.0197529 0.711 16 Infrared 1E+18 1.192 BK_7 1.517 64.2 rays filter 17 1E+18 0.812 18 Image 1E+18 −0.004 plane Reference wavelength: 555 nm; the position of blocking light: the effective half diameter of the clear aperture of the seventh surface is 4.300 mm.

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5605 0.2260 0.4213 0.3124 0.2140 0.2302 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2166 1.5244 0.6567 2.3214 1.2002 0.3534 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.4033 1.8640 1.1124 0.8972 HOS InTL HOS/HOI InS/HOS ODT % TDT % 38.9997 36.2894 7.7999 0.5580 −75.5513 49.1462 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTA NSTA NLTA SSTA SLTA −0.007 mm 0.003 mm −0.035 mm −0.041 mm −0.005 mm −0.010 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.010 −0.010 −0.000 −0.010 −0.015 −0.010 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.705 0.720 0.665 0.705 0.469 0.121 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 −0.010 −0.010 −0.000 −0.010 −0.005 0.010 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.680 0.743 0.587 0.680 0.765 0.547 FS AIFS AVFS AFS 0.000 −0.004 −0.009 0.005

The figures related to the profile curve lengths obtained based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 0.999 1.000 0.00019 100.02% 4.582 21.82% 12 0.999 1.010 0.01033 101.03% 4.582 22.04% 21 0.999 0.999 −0.00010 99.99% 8.000 12.49% 22 0.999 1.000 0.00094 100.09% 8.000 12.50% 31 0.999 1.000 0.00008 100.01% 3.663 27.29% 32 0.999 1.005 0.00585 100.58% 3.663 27.44% 41 0.999 1.006 0.00627 100.63% 2.000 50.29% 42 0.999 1.000 0.00105 100.11% 2.000 50.02% 51 0.999 0.999 −0.00039 99.96% 3.890 25.68% 52 0.999 1.001 0.00146 100.15% 3.890 25.73% 61 0.999 1.001 0.00146 100.15% 3.646 27.45% 62 0.999 0.999 −0.00038 94.96% 3.646 27.40% 71 0.999 1.000 0.00027 100.03% 2.000 49.99% 72 0.999 0.999 −0.00043 99.96% 2.000 49.95% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 11.096 12.187 1.09113 109.83% 4.582 266.00% 12 3.979 6.019 2.04015 151.27% 4.582 131.38% 21 3.872 3.891 0.01907 100.49% 8.000 48.63% 22 2.951 2.986 0.03546 101.20% 8.000 37.33% 31 3.211 3.228 0.01696 100.53% 3.663 88.13% 32 3.519 3.866 0.34704 109.86% 3.663 105.54% 41 3.451 3.804 0.35317 110.23% 2.000 190.21% 42 4.300 4.426 0.12640 102.94% 2.000 221.32% 51 4.884 4.888 0.00390 100.08% 3.890 125.66% 52 5.405 5.758 0.35382 106.55% 3.890 148.02% 61 5.628 6.034 0.40595 107.21% 3.646 165.49% 62 5.113 5.120 0.00612 100.12% 3.646 140.41% 71 5.036 5.130 0.09388 101.86% 2.000 256.51% 72 5.054 5.054 −0.00035 99.99% 2.000 252.68%

The results of the equations of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment (Reference wavelength: 555 nm) HIF211 0 HIF211/HOI 0 SGI211 0 |SGI211|/ 0 (|SGI211| + TP2)

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system of the sixth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a sixth lens 660, a seventh lens 670, an infrared rays filter 680, an image plane 690, and an image sensor 692. FIG. 6C shows a transverse aberration diagram at 0.7 field of view of the sixth embodiment of the present invention. FIG. 6D is a diagram showing the through-focus MTF values of the visible light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present invention. FIG. 6E is a diagram showing the through-focus MTF values of the infrared light spectrum at the central field of view, 0.3 field of view, and 0.7 field of view of the sixth embodiment of the present disclosure. Lights of any field of view of the present disclosure can be further divided into sagittal ray and tangential ray, and the spatial frequency of 55 cycles/mm serves as the benchmark for assessing the focus shifts and the values of MTF. A wavelength of the infrared light is 850 nm.

The first lens 610 has negative refractive power and is made of glass. An object-side surface 612, which faces the object side, is a convex spherical surface, and an image-side surface 614, which faces the image side, is a concave spherical surface.

The second lens 620 has positive refractive power and is made of glass. An object-side surface 622 thereof, which faces the object side, is a concave spherical surface, and an image-side surface 624 thereof, which faces the image side, is a convex spherical surface.

The third lens 630 has negative refractive power and is made of glass. An object-side surface 632, which faces the object side, is a concave spherical surface, and an image-side surface 634, which faces the image side, is a convex spherical surface.

The fourth lens 640 has positive refractive power and is made of glass. An object-side surface 642, which faces the object side, is a convex spherical surface, and an image-side surface 644, which faces the image side, is a convex spherical surface.

The fifth lens 650 has negative refractive power and is made of glass. An object-side surface 652, which faces the object side, is a convex spherical surface, and an image-side surface 654, which faces the image side, is a concave spherical surface.

The sixth lens 660 has positive refractive power and is made of glass. An object-side surface 662, which faces the object side, is a convex spherical surface, and an image-side surface 664, which faces the image side, is a convex spherical surface. Whereby, the incident angle of each view field could be adjusted to improve aberration.

The seventh lens 670 has positive refractive power and is made of glass. An object-side surface 672, which faces the object side, is a convex spherical surface, and an image-side surface 674, which faces the image side, is a convex spherical surface. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventh lens 670 and the image plane 690. The infrared rays filter 680 gives no contribution to the focal length of the system.

The parameters of the lenses of the sixth embodiment are listed in Table 11 and Table 12.

TABLE 11 f = 4.8139 mm; f/HEP = 1.8; HAF = 70 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object 1E+18 1E+18 1 1^(st) lens 39.54933668 2.000 glass 1.517 64.20 −8.869671 2 3.989012795 6.415 3 Aperture 1E+18 0.336 glass 4 2^(nd) lens −22.16007528 5.345 2.001 29.13 7.063128 5 −5.879601349 0.368 glass 6 3^(rd) lens −5.312833715 2.000 2.002 19.32 −13.152696 7 −10.83074836 0.200 8 4^(th) lens 22.42820063 3.625 glass 1.497 81.56 20.450187 9 −17.23453558 0.200 10 5^(th) lens 53.79157428 2.000 glass 2.002 19.32 −23.669587 11 15.73460584 0.650 12 6^(th) lens 25.68653381 4.165 glass 1.497 81.56 20.722828 13 −15.96786491 0.200 14 7^(th) lens 12.16681759 6.490 glass 1.497 81.56 23.579801 15 −200.02 3.007 16 Infrared 1E+18 1.000 BK_7 1.517 64.2 rays filter 17 1E+18 1.001 18 Image 1E+18 −0.001 plane Reference wavelength: 555 nm; the position of blocking light: the effective half diameter of the clear aperture of the seventh surface is 4.500 mm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the sixth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5516 0.7056 0.3816 0.2386 0.2130 0.2355 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2070 1.6204 0.9126 1.7755 1.4025 0.0415 |f1/f2| |f2/f3| (TP7 + IN12)/TP2 (TP7 + IN67)/TP6 1.2793 0.5408 1.6374 1.6062 HOS InTL HOS/HOI InS/HOS ODT % TDT % 39.0001 33.9934 7.8000 0.7842 −62.2276 43.7400 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 PSTA PLTA NSTA NLTA SSTA SLTA 0.013 mm 0.000 mm 0.043 mm 0.044 mm 0.023 mm 0.013 mm VSFS0 VSFS3 VSFS7 VTFS0 VTFS3 VTFS7 −0.010 −0.015 −0.020 −0.010 −0.010 0.010 VSMTF0 VSMTF3 VSMTF7 VTMTF0 VTMTF3 VTMTF7 0.814 0.643 0.547 0.814 0.417 0.127 ISFS0 ISFS3 ISFS7 ITFS0 ITFS3 ITFS7 −0.010 −0.015 −0.025 −0.010 −0.015 −0.010 ISMTF0 ISMTF3 ISMTF7 ITMTF0 ITMTF3 ITMTF7 0.834 0.747 0.436 0.834 0.736 0.468 FS AIFS AVFS AFS 0.000 −0.014 −0.009 0.005

The figures related to the profile curve lengths obtained based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.351 1.351 −0.00014 99.99% 2.000 67.56% 12 1.351 1.378 0.02686 101.99% 2.000 68.91% 21 1.351 1.352 0.00044 100.03% 5.345 25.29% 22 1.351 1.363 0.01178 100.87% 5.345 25.51% 31 1.351 1.366 0.01460 101.08% 2.000 68.30% 32 1.351 1.355 0.00313 100.23% 2.000 67.73% 41 1.351 1.352 0.00042 100.03% 3.625 37.30% 42 1.351 1.352 0.00099 100.07% 3.625 37.31% 51 1.351 1.351 −0.00026 99.98% 2.000 67.56% 52 1.351 1.353 0.00127 100.09% 2.000 67.63% 61 1.351 1.352 0.00022 100.02% 4.165 32.45% 62 1.351 1.353 0.00122 100.09% 4.165 32.48% 71 1.351 1.354 0.00239 100.18% 6.490 20.86% 72 1.351 1.351 −0.00039 99.97% 6.490 20.82% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 8.312 8.373 0.06190 100.74% 2.000 418.67% 12 3.904 5.436 1.53234 139.25% 2.000 271.80% 21 2.446 2.450 0.00413 100.17% 5.345 45.84% 22 3.606 3.881 0.27480 107.62% 5.345 72.61% 31 3.595 3.949 0.35347 109.83% 2.000 197.43% 32 4.500 4.641 0.14070 103.13% 2.000 232.04% 41 5.438 5.493 0.05468 101.01% 3.625 151.54% 42 5.808 5.923 0.11519 101.98% 3.625 163.41% 51 5.977 5.989 0.01205 100.20% 2.000 299.47% 52 5.979 6.132 0.15347 102.57% 2.000 306.60% 61 6.076 6.133 0.05760 100.95% 4.165 147.25% 62 6.500 6.693 0.19362 102.98% 4.165 160.70% 71 6.850 7.275 0.42507 106.21% 6.490 112.09% 72 6.177 6.177 0.00006 100.00% 6.490 95.18%

The results of the equations of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment (Reference wavelenth: 555 nm) HIF211 0 HIF211/HOI 0 SGI211 0 |SGI211|/ 0 (|SGI211| + TP2)

It must be pointed out that the embodiments described above are only some embodiments of the present invention. All equivalent structures which employ the concepts disclosed in this specification and the appended claims should fall within the scope of the present invention. 

What is claimed is:
 1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; a first image plane, which is an image plane specifically for visible light and perpendicular to the optical axis; a through-focus modulation transfer rate (value of MTF) at a first spatial frequency having a maximum value at central field of view of the first image plane; and a second image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency having a maximum value at central of field of view of the second image plane; wherein the optical image capturing system consists of the seven lenses with refractive power; at least one lens among the first lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; |FS|≤60 μm; and 1≤HOS/HOI≤15; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance between an object-side surface of the first lens and the first image plane on the optical axis; HOI is a maximum image height on the first image plane perpendicular to the optical axis; InTL is a distance on the optical axis from the object-side surface of the first lens to the image-side surface of the seventh lens; HAF is a half of a maximum view angle of the optical image capturing system; for any surface of any lens; FS is a distance on the optical axis between the first image plane and the second image plane.
 2. The optical image capturing system of claim 1, wherein a wavelength of the infrared light ranges from 700 nm to 1300 nm, and the first spatial frequency is denoted by SP1, which satisfies the following condition: SP1≤440 cycles/mm.
 3. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 1≤HOS/HOI≤15.
 4. The optical image capturing system of claim 1, wherein at least one lens among the first lens to the seventh lens is made of glass.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: |FS|≤10 μm.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 1≤2(ARE/HEP)≤2.0; where ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.05≤ARE71/TP7≤35; and 0.05≤ARE72/TP7≤35; where ARE71 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the seventh lens, along a surface profile of the object-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE72 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the seventh lens, along a surface profile of the image-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 8. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: PLTA≤100 μm; PSTA≤100 μm; NLTA≤100 μm; NSTA≤100 μm; SLTA≤100 μm; SSTA≤100 μm; and |TDT|<250%; where TDT is a TV distortion; PLTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength passing through an edge of the aperture; PSTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of the tangential fan after a shortest operation wavelength passing through the edge of the aperture; NLTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the longest operation wavelength passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the shortest operation wavelength passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan of the optical image capturing system after the longest operation wavelength passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan after the shortest operation wavelength passing through the edge of the aperture.
 9. The optical image capturing system of claim 1, further comprising an aperture, wherein a wavelength of the infrared light ranges from 700 nm to 1300 nm, and the first spatial frequency is denoted by SP1, which satisfies the following condition: 0.25≤InS/HOS≤1.1; and SP1≤55 cycles/mm; where InS is a distance between the aperture and the first image plane on the optical axis.
 10. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; a first image plane, which is an image plane specifically for visible light and perpendicular to the optical axis; a through-focus modulation transfer rate (value of MTF) at a first spatial frequency having a maximum value at central field of view of the first image plane, and the first spatial frequency being 55 cycles/mm; and a second image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the through-focus modulation transfer rate (value of MTF) at the first spatial frequency having a maximum value at central of field of view of the second image plane, and the first spatial frequency being 55 cycles/mm; wherein the optical image capturing system consists of the seven lenses with refractive power; at least one lens among the first lens to the seventh lens is made of glass; at least one lens among the first lens to the seventh lens has positive refractive power; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1.0≤f/HEP≤10.0; 0 deg<HAF≤150 deg; |FS|≤30 μm; 1≤2(ARE/HEP)≤2.0; and 1≤HOS/HOI≤15; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance between the object-side surface of the first lens and the first image plane on the optical axis; InTL is a distance on the optical axis from the object-side surface of the first lens to the image-side surface of the seventh lens; HAF is a half of a maximum view angle of the optical image capturing system; for any surface of any lens; FS is a distance on the optical axis between the first image plane and the second image plane; ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 11. The optical image capturing system of claim 10, wherein each two neighboring lenses among the first to the seventh lenses are separated by air.
 12. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 1≤ARS/EHD≤2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 13. The optical image capturing system of claim 10, wherein at least one lens among the first lens to the sixth lens is made of glass, and the lens made of glass is aspheric surface.
 14. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: |FS|≤10 μm.
 15. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 1≤HOS/HOI≤10.
 16. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: IN34+IN45≤TP3; IN34+IN45≤TP4; and IN34+IN45≤TP5; where IN34 is a distance on the optical axis between the third lens and the fourth lens; IN45 is a distance on the optical axis between the fourth lens and the fifth lens; TP3 is a thickness of the third lens on the optical axis; TP4 is a thickness of the fourth lens on the optical axis; TP5 is a thickness of the fifth lens on the optical axis.
 17. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0≤IN67/f≤5.0; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens.
 18. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.1≤(TP7+IN67)/TP6≤50; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens; TP6 is a thickness of the sixth lens on the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 19. The optical image capturing system of claim 10, wherein at least one lens among the first lens to the seventh lens is a light filter, which is capable of filtering out light of wavelengths shorter than 500 nm.
 20. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; a first average image plane, which is an image plane specifically for visible light and perpendicular to the optical axis; the first average image plane being installed at the average position of the defocusing positions, where through-focus modulation transfer rates (values of MTF) of the visible light at central field of view, 0.3 field of view, and 0.7 field of view are at their respective maximum at a first spatial frequency; the first spatial frequency being 55 cycles/mm; and a second average image plane, which is an image plane specifically for infrared light and perpendicular to the optical axis; the second average image plane being installed at the average position of the defocusing positions, where through-focus modulation transfer rates of the infrared light (values of MTF) at central field of view, 0.3 field of view, and 0.7 field of view are at their respective maximum at the first spatial frequency; the first spatial frequency being 55 cycles/mm; wherein the optical image capturing system consists of the seven lenses having refractive power; at least one lens among the first lens to the seventh lens is made of glass; each lens among the first lens to the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side; wherein the optical image capturing system satisfies: 1≤f/HEP≤0; 0 deg<HAF≤150 deg; |AFS|≤30 μm; 1≤2(ARE/HEP)≤2.0; and 1≤HOS/HOI≤10; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of a maximum view angle of the optical image capturing system; HOS is a distance between an object-side surface of the first lens and the image plane on the optical axis; HOI is a maximum image height on the first image plane perpendicular to the optical axis; InTL is a distance on the optical axis from the object-side surface of the first lens to the image-side surface of the seventh lens; AFS is a distance on the optical axis between the first average image plane and the second average image plane; ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 1≤ARS/EHD≤2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 22. The optical image capturing system of claim 20, wherein all of the first lens to the seventh lens are made of glass.
 23. The optical image capturing system of claim 20, wherein at least one surface of at least one lens among the first lens to the seventh lens is aspheric surface.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: |AFS|≤30 μm.
 25. The optical image capturing system of claim 20, further comprising an aperture and an image sensor, wherein the image sensing device is disposed on the first average image plane and comprises at least 100 thousand pixels; the optical image capturing system further satisfies: 0.2≤InS/HOS≤1.1; where InS is a distance between the aperture and the first average image plane on the optical axis. 